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JPH0820225B2 - A device for measuring the diameter or width of thin wires - Google Patents
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JPH0820225B2 - A device for measuring the diameter or width of thin wires - Google Patents

A device for measuring the diameter or width of thin wires

Info

Publication number
JPH0820225B2
JPH0820225B2 JP4213226A JP21322692A JPH0820225B2 JP H0820225 B2 JPH0820225 B2 JP H0820225B2 JP 4213226 A JP4213226 A JP 4213226A JP 21322692 A JP21322692 A JP 21322692A JP H0820225 B2 JPH0820225 B2 JP H0820225B2
Authority
JP
Japan
Prior art keywords
width
diameter
lens
measured
linear object
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP4213226A
Other languages
Japanese (ja)
Other versions
JPH06117825A (en
Inventor
茂 林
正司 堀内
Original Assignee
科学技術庁航空宇宙技術研究所長
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by 科学技術庁航空宇宙技術研究所長 filed Critical 科学技術庁航空宇宙技術研究所長
Priority to JP4213226A priority Critical patent/JPH0820225B2/en
Publication of JPH06117825A publication Critical patent/JPH06117825A/en
Publication of JPH0820225B2 publication Critical patent/JPH0820225B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Length Measuring Devices By Optical Means (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】従来、細い線の径あるいは幅の寸
法を非接触的に測定する装置としては、被測定物体の寸
法よりも幅の広い平面状の平行なビーム中に、該ビーム
平面と直角に被測定物体を挿入し、これによって生じる
影の幅を、光電変換素子を直線状に配列したイメージセ
ンサー等によって検出測定する装置、あるいは細いレー
ザービームが一定速度で走査する空間に、そのレーザー
ビームの走査面と直角に被測定物体を挿入し、そのレー
ザービームが遮蔽される時間と走査速度とから線径を測
定する装置が使用されている。これらの装置は、高速か
つ非接触に物体の寸法を測定できるので製品検査の分野
において広く使用されている。
BACKGROUND OF THE INVENTION Conventionally, an apparatus for contactlessly measuring the diameter or width of a thin wire has been known in which a plane parallel beam having a width wider than the dimension of an object to be measured is used. Insert the object to be measured at a right angle to, and measure the width of the shadow generated by this with an image sensor, etc. in which photoelectric conversion elements are linearly arranged, or in a space where a thin laser beam scans at a constant speed, There is used a device in which an object to be measured is inserted at a right angle to a scanning surface of a laser beam and a wire diameter is measured from a time when the laser beam is shielded and a scanning speed. These devices are widely used in the field of product inspection because they can measure the dimensions of objects at high speed and in a non-contact manner.

【0002】[0002]

【発明が解決しようとする課題】しかしながら、これら
の従来の装置は、被測定物体の寸法が数十マイクロメー
タ以下になると、物体の縁での回折現象のために光が被
測定物体の背後に回り込むため、高い精度での測定が困
難となるという問題があった。本発明は、この回折現象
を利用することによって、主として太さ、あるいは幅が
数十ミクロン以下の線状物体や帯状物体の寸法を高い精
度で測定するための方法と装置を提供する。
However, in these conventional devices, when the size of the object to be measured becomes several tens of micrometers or less, light is reflected behind the object to be measured due to the diffraction phenomenon at the edge of the object. Since it goes around, there is a problem that it is difficult to perform measurement with high accuracy. The present invention provides a method and an apparatus for measuring the dimension of a linear object or a band-shaped object whose thickness or width is several tens of microns or less with high accuracy by utilizing this diffraction phenomenon.

【0003】[0003]

【課題を解決するための手段】上記目的を達成する本発
明の線状物体の直径あるいは寸法測定方法は、被測定線
状物体にその幅よりも大きい幅を有する単色平行ビーム
を照射し、その散乱光をレンズで集束し、fをレンズの
焦点距離、rを焦点面における焦点からの距離、I(r/
f)をr/fにおける焦点面上の散乱光の強度としたと
き、I(r/f)・(r/f)が最大となる位置から被測
定線状物体の径或いは幅Dを求めることを特徴とする。
また、距離rにおける散乱光のエネルギーの理論値Ert
と実測値Ermとの誤差の二乗の和Σ(Erm−Ert)2
最小とするようなDの値を求めることによっても径或い
は幅Dを得ることが出来る。
The diameter or dimension measuring method of a linear object of the present invention which achieves the above object is to irradiate a linear object to be measured with a monochromatic parallel beam having a width larger than the width of the linear object. The scattered light is focused by the lens, f is the focal length of the lens, r is the distance from the focal point in the focal plane, and I (r /
When f) is the intensity of scattered light on the focal plane at r / f, obtain the diameter or width D of the linear object to be measured from the position where I (r / f) · (r / f) is maximum. Is characterized by.
Further, the theoretical value Ert of the energy of scattered light at the distance r
The diameter or width D can also be obtained by obtaining the value of D that minimizes the sum Σ (Erm−Ert) 2 of the error between the measured value Erm and the measured value Erm.

【0004】[0004]

【作用】測定の原理を図1に基づいて簡単に説明する。
径あるいは幅がDの被測定線状物体1に、その幅dが幅
Dよりも大きい単色の平行ビーム2を照射し、その散乱
光3をレンズ4で集める。このレンズの焦点面5におけ
る散乱光の強度分布Iは、 I(r/f)=D2sin2{(πD/λ)(r/f)}/{(πD/λ)(r/f)2} で表わされ、図1(b)の実線で示すようになる。λは
照射する単色光の波長、fはレンズの焦点距離、rは焦
点面における焦点からの距離である。この強度分布にr
/fをかけて得られるI(r/f)・(r/f)は理論計
算によると、同図中に点線で示すように、r/f=1.
165/(πD/λ)において極大となる。この極大の位
置はDの大きさによって一義的にきまる。このことを利
用すれば、光電変換素子を配列したアレーによって得ら
れる散乱強度信号から、散乱強度が最大となる距離rが
得られ、これから寸法Dを決定できる。あるいは、配列
のi番目の素子の受ける散乱光のエネルギーをEi と
し、理論値Eitと実測値Eimとがもっともよく一致する
ように、たとえば、誤差の二乗の和Σ(Eim−Eit)2
を最小とするようなDの値を繰り返し求めることによっ
て線径Dを決定することができる。
The principle of measurement will be briefly described with reference to FIG.
A linear object 2 having a diameter or width D is irradiated with a monochromatic parallel beam 2 having a width d larger than the width D, and scattered light 3 is collected by a lens 4. The intensity distribution I of the scattered light on the focal plane 5 of this lens is I (r / f) = D 2 sin 2 {(πD / λ) (r / f)} / {(πD / λ) (r / f) 2 }, as shown by the solid line in FIG. λ is the wavelength of the monochromatic light emitted, f is the focal length of the lens, and r is the distance from the focal point on the focal plane. R to this intensity distribution
According to theoretical calculation, I (r / f)  (r / f) obtained by multiplying / f is r / f = 1.
It becomes a maximum at 165 / (πD / λ). The position of this maximum is uniquely determined by the size of D. By utilizing this, the distance r at which the scattering intensity is maximum can be obtained from the scattering intensity signal obtained by the array in which the photoelectric conversion elements are arranged, and the dimension D can be determined from this. Alternatively, the energy of scattered light received by the i-th element of the array is set to Ei, and the theoretical value Eit and the measured value Eim are best matched, for example, the sum of squared errors Σ (Eim−Eit) 2
The wire diameter D can be determined by repeatedly obtaining the value of D that minimizes

【0005】[0005]

【実施例】本発明の線状物体の直径あるいは寸法測定装
置の実施例を図2に示す。平行なレーザービーム11に
よって細線(被測定物体)12を照射し、この細線によ
る散乱光13を受光レンズ14により焦点Oに集束す
る。このレンズの焦点面には部分環状光電変換素子18
のアレー19が置かれている。各素子18の電流は信号
処理器15で電圧信号に変換され、16の演算器におい
て上述の方法で線径の大きさが計算され、表示器17に
表示される。散乱光の強度を検出するセンサー18はリ
ニアーアレーでもよいが、この場合、被測定物体が素子
の配列の方向と垂直になるように保持する必要がある。
図示のようにリング状の光電変換素子19を配列したセ
ンサーを使用すれば、被測定物体12を特定方向に保つ
必要がない。このリング状の光電変換素子は、焦点Oに
対して360°をカバーする必要はなく、実用的にはθ
=45°程度をカバーする部分環状光電変換素子であれ
ば良い。
EXAMPLE FIG. 2 shows an example of the apparatus for measuring the diameter or dimension of a linear object according to the present invention. A parallel laser beam 11 irradiates a fine line (object to be measured) 12, and scattered light 13 by the fine line is focused on a focus O by a light receiving lens 14. The partial annular photoelectric conversion element 18 is provided on the focal plane of this lens.
Array 19 of is placed. The current of each element 18 is converted into a voltage signal by the signal processor 15, the size of the wire diameter is calculated by the above-mentioned method in the calculator of 16 and displayed on the display unit 17. The sensor 18 for detecting the intensity of scattered light may be a linear array, but in this case, it is necessary to hold the measured object so that it is perpendicular to the direction of the array of elements.
If the sensor in which the ring-shaped photoelectric conversion elements 19 are arranged as shown in the figure is used, it is not necessary to keep the measured object 12 in a specific direction. This ring-shaped photoelectric conversion element does not need to cover 360 ° with respect to the focal point O, and θ is practically used.
Any partial annular photoelectric conversion element that covers about 45 ° may be used.

【0006】[0006]

【発明の効果】本発明の方法および装置による測定例を
図3に示す。(a)は18μm、(b)は25μm、
(c)は30μmの細線の測定例であり、理論値を示す
点線と、測定値を示す実線とは良く一致し、容易に線径
を求めることが出来る。本発明は、上記のように従来の
測定法では測定精度を低下させる原因であった回折現象
を積極的に利用し、簡単な装置によって、従来困難であ
った数十ミクロン以下の線状或いは帯状体の幅を精度良
く測定出来たものである。
FIG. 3 shows an example of measurement by the method and apparatus of the present invention. (A) is 18 μm, (b) is 25 μm,
(C) is a measurement example of a thin line of 30 μm, and the dotted line showing the theoretical value and the solid line showing the measured value are in good agreement, and the wire diameter can be easily obtained. INDUSTRIAL APPLICABILITY As described above, the present invention positively utilizes the diffraction phenomenon which has been a cause of lowering the measurement accuracy in the conventional measurement method, and uses a simple device to form a linear or strip-like shape of several tens of microns or less, which has been difficult in the past. I was able to measure the width of my body accurately.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の細線の径あるいは幅を測定する測定原
理を示す説明図である。
FIG. 1 is an explanatory diagram showing a measurement principle for measuring the diameter or width of a thin wire of the present invention.

【図2】本発明の細線の径あるいは幅を測定する装置の
1実施例の構成を示す概念図である。
FIG. 2 is a conceptual diagram showing the configuration of one embodiment of an apparatus for measuring the diameter or width of a thin wire of the present invention.

【図3】上記実施例装置による測定値を示すグラフであ
る。
FIG. 3 is a graph showing measured values by the apparatus of the above-mentioned embodiment.

【符号の説明】[Explanation of symbols]

1,12 被測定対象細線 2,11 レーザ
ービーム 3,13 散乱光 4,14 レンズ 5 焦点面 15 信号処理器 16 演算器 17 表示器 18 光電変換素子 19 センサーア
レー
1, 12 thin line to be measured 2, 11 laser beam 3, 13 scattered light 4, 14 lens 5 focal plane 15 signal processor 16 calculator 17 display 18 photoelectric conversion element 19 sensor array

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 被測定線状物体にその幅よりも大きい幅
を有する単色平行ビームを照射し、その散乱光をレンズ
で集束し、fをレンズの焦点距離、rを焦点面における
焦点からの距離、I(r/f)をr/fにおける焦点面上
の散乱光の強度としたとき、I(r/f)・(r/f)が
最大となる位置から被測定線状物体の径或いは幅Dを求
めることを特徴とする細い線の径あるいは幅を測定する
方法
1. A linear object to be measured is irradiated with a monochromatic parallel beam having a width larger than its width, the scattered light is focused by a lens, f is the focal length of the lens, and r is the focal point from the focal plane. When the distance and I (r / f) are the intensity of scattered light on the focal plane at r / f, the diameter of the linear object to be measured is measured from the position where I (r / f) · (r / f) is maximum. Alternatively, a method for measuring the diameter or width of a thin line characterized by obtaining the width D
【請求項2】 被測定線状物体にその幅よりも大きい幅
を有する単色平行ビームを照射し、その散乱光をレンズ
で集束し、fをレンズの焦点距離、rを焦点面における
焦点からの距離としたとき、距離rにおける散乱光のエ
ネルギーの理論値Ertと実測値Ermとの誤差の二乗の和
Σ(Erm−Ert)2を最小とするようなDの値を求める
ことを特徴とする細い線の径あるいは幅を測定する方法
2. A linear object to be measured is irradiated with a monochromatic parallel beam having a width larger than its width, the scattered light is focused by a lens, f is the focal length of the lens, r is the focal point from the focal plane. When the distance is defined as a distance, the value of D that minimizes the sum Σ (Erm−Ert) 2 of the error between the theoretical value Ert of the scattered light energy and the measured value Erm at the distance r is characterized. How to measure the diameter or width of thin wires
【請求項3】 単色光源と、該光源からの平行ビームに
よって照射される被測定線状物体と、該線状物体から散
乱される光を受光するレンズと、その光学レンズの焦点
に配置された光電変換素子アレーと、それらの素子から
の電流信号を検出する装置と、得られた強度分布を解析
する装置及び線径を表示する表示器とからなり、該解析
装置はfをレンズの焦点距離、rを焦点面における焦点
からの距離、I(r/f)をr/fにおける焦点面上の
散乱光の強度としたとき、I(r/f)・(r/f)を
求める演算回路及び得られたI(r/f)・(r/f)
が最大となるr/fを求める演算回路を含むことを特
徴とする線状物体の径あるいは幅を測定する装置
3. A monochromatic light source, a linear object to be measured illuminated by a parallel beam from the light source, a lens for receiving light scattered from the linear object, and a focal point of the optical lens. consists of a photoelectric conversion element array, means for sensing current signals from these elements, the display for displaying the device and wire diameter for analyzing the resulting intensity distribution, the analysis
The device is f the focal length of the lens, r the focal point in the focal plane
Distance from, I (r / f) on the focal plane at r / f
When the intensity of scattered light is I (r / f) · (r / f),
Arithmetic circuit to be obtained and obtained I (r / f) · (r / f)
It includes an arithmetic circuit that calculates r / f that maximizes
Apparatus for measuring the diameter or width of the linear object to symptoms
【請求項4】 上記光電変換素子アレーが、部分環状光
電変換素子であることを特徴とする請求項3の線状物体
の直径あるいは寸法測定装置
4. The linear object diameter or size measuring device according to claim 3, wherein the photoelectric conversion element array is a partial annular photoelectric conversion element.
JP4213226A 1992-07-20 1992-07-20 A device for measuring the diameter or width of thin wires Expired - Lifetime JPH0820225B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4213226A JPH0820225B2 (en) 1992-07-20 1992-07-20 A device for measuring the diameter or width of thin wires

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4213226A JPH0820225B2 (en) 1992-07-20 1992-07-20 A device for measuring the diameter or width of thin wires

Publications (2)

Publication Number Publication Date
JPH06117825A JPH06117825A (en) 1994-04-28
JPH0820225B2 true JPH0820225B2 (en) 1996-03-04

Family

ID=16635628

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4213226A Expired - Lifetime JPH0820225B2 (en) 1992-07-20 1992-07-20 A device for measuring the diameter or width of thin wires

Country Status (1)

Country Link
JP (1) JPH0820225B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3611140B2 (en) * 1995-07-20 2005-01-19 計測器工業株式会社 Yarn measuring device
JP4509593B2 (en) * 2004-02-13 2010-07-21 株式会社山武 Detection method of rod runout

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3164559D1 (en) * 1980-07-16 1984-08-09 Davy Mckee Sheffield Rolling mills
JPS5744407U (en) * 1980-08-28 1982-03-11
JPH0629859B2 (en) * 1986-01-14 1994-04-20 株式会社神戸製鋼所 Surface defect detector
JPH0623921Y2 (en) * 1988-02-15 1994-06-22 株式会社島津製作所 Ring detector

Also Published As

Publication number Publication date
JPH06117825A (en) 1994-04-28

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